Line Integrals of Scalar Fields - Calculus 3

  1. Consider two curves: C1C_1 is the straight line from (0,0,0)(0,0,0) to (1,1,1)(1,1,1), and C2C_2 is the curve parameterized by r(t)=(t,t2,t3)\mathbf{r}(t) = (t, t^2, t^3) for 0≤t≤10 \leq t \leq 1. Both curves connect the same endpoints. If f(x,y,z)=x2+y2+z2f(x,y,z) = x^2 + y^2 + z^2, which statement about the line integrals ∫C1f ds\int_{C_1} f \, ds and ∫C2f ds\int_{C_2} f \, ds is correct?
    Answer: The relationship depends on the specific values computed for each integral Line integrals of scalar fields are path-dependent and depend on both the function values along the path and the arc length element. For C1C_1: r1(t)=(t,t,t)\mathbf{r}_1(t) = (t,t,t) for t∈[0,1]t \in [0,1], so ∣r1′(t)∣=3|\mathbf{r}_1'(t)| = \sqrt{3} and f(r1(t))=3t2f(\mathbf{r}_1(t)) = 3t^2. Thus ∫C1f ds=3∫013t2 dt=3\int_{C_1} f \, ds = \sqrt{3}\int_0^1 3t^2 \, dt = \sqrt{3}. For C2C_2: r2(t)=(t,t2,t3)\mathbf{r}_2(t) = (t,t^2,t^3) for t∈[0,1]t \in [0,1], so ∣r2′(t)∣=1+4t2+9t4|\mathbf{r}_2'(t)| = \sqrt{1 + 4t^2 + 9t^4} and f(r2(t))=t2+t4+t6f(\mathbf{r}_2(t)) = t^2 + t^4 + t^6. The integral ∫C2f ds=∫01(t2+t4+t6)1+4t2+9t4 dt\int_{C_2} f \, ds = \int_0^1 (t^2 + t^4 + t^6)\sqrt{1 + 4t^2 + 9t^4} \, dt is more complex but computable. Option A is wrong because shorter arc length doesn't guarantee larger integral value. Option B is wrong because longer arc length doesn't guarantee larger integral value either - the function values matter. Option C is wrong because line integrals of scalar fields are path-dependent (unlike line integrals of conservative vector fields). Option D is correct because we need to compute both integrals to determine their relationship.
  2. The work done by a force field F(x,y,z)=(y,x,z2)\mathbf{F}(x,y,z) = (y, x, z^2) in moving a particle along the curve r(t)=(cos⁡t,sin⁡t,t)\mathbf{r}(t) = (\cos t, \sin t, t) from t=0t = 0 to t=πt = \pi is equal to the line integral of which scalar field over the same curve?
    Answer: f(x,y,z)=(sin⁡t)(−sin⁡t)+(cos⁡t)(cos⁡t)+t2(1)f(x,y,z) = (\sin t)(-\sin t) + (\cos t)(\cos t) + t^2(1) Work is computed as ∫CF⋅dr=∫abF(r(t))⋅r′(t) dt\int_C \mathbf{F} \cdot d\mathbf{r} = \int_a^b \mathbf{F}(\mathbf{r}(t)) \cdot \mathbf{r}'(t) \, dt. Here, F(r(t))=(sin⁡t,cos⁡t,t2)\mathbf{F}(\mathbf{r}(t)) = (\sin t, \cos t, t^2) and r′(t)=(−sin⁡t,cos⁡t,1)\mathbf{r}'(t) = (-\sin t, \cos t, 1). The dot product is F⋅r′=(sin⁡t)(−sin⁡t)+(cos⁡t)(cos⁡t)+t2(1)=−sin⁡2t+cos⁡2t+t2=cos⁡(2t)+t2\mathbf{F} \cdot \mathbf{r}' = (\sin t)(-\sin t) + (\cos t)(\cos t) + t^2(1) = -\sin^2 t + \cos^2 t + t^2 = \cos(2t) + t^2. This equals the line integral ∫Cf ds\int_C f \, ds where ff is the scalar field that, when evaluated along the curve and multiplied by ds/dt=∣r′(t)∣ds/dt = |\mathbf{r}'(t)|, gives the same integrand. But more directly, the work integral ∫0π(sin⁡t)(−sin⁡t)+(cos⁡t)(cos⁡t)+t2(1) dt\int_0^\pi (\sin t)(-\sin t) + (\cos t)(\cos t) + t^2(1) \, dt matches option D exactly. The other options incorrectly represent the relationship between work and line integrals of scalar fields.

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